ライフサイエンスコーパス: diffraction

1 spectroscopy as well as single-crystal X-ray diffraction.

2 then established using single crystal X-ray diffraction.

3 d on the basis of NMR measurements and X-ray diffraction.

4 d can be timed to initiate a reaction before diffraction.

5 spersive X-ray spectroscopy and powder X-ray diffraction.

6 bution function (PDF) obtained from electron diffraction.

7 tering patterns that are overlaid with Bragg diffraction.

8 e were detected by NMR and synchrotron X-ray diffraction.

9 change reaction using in situ powder neutron diffraction.

10 d crystals were determined with powder X-ray diffraction.

11 electronic absorption spectroscopy and X-ray diffraction.

12 r solving the phase problem in X-ray crystal diffraction.

13 Most complexes were characterized by X-ray diffraction.

14 glass up to 172 GPa using high-energy X-ray diffraction.

15 alloys during heating by in situ synchrotron diffraction.

16 through wavefront reconstruction by means of diffraction.

17 by in situ variable temperature powder X-ray diffraction.

18 ransmission electron microscopy and electron diffraction.

19 interference effect analogous to multi-slit diffraction.

20 were analyzed using synchrotron-based X-ray diffraction.

21 ing small-angle neutron scattering and X-ray diffraction.

22 tures were confirmed by single-crystal X-ray diffraction.

23 , UV-vis, EPR, NMR, and single-crystal X-ray diffractions.

24 ns are characterized by single-crystal X-ray diffraction, (1)H and (13)C NMR, and negative-ion ESI-MS

25 NMR, ESR, and neutron diffraction allow the environment of the solvated electr

26 Ultrafast X-ray diffraction allows the direct imaging of atomic dynamics

27 ar dichroism (ECD), and single-crystal X-ray diffraction analyses.

28 Using single-crystal X-ray diffraction analysis (SCXRD), we show that the phase cha

29 The (11)B NMR spectrum, X-ray diffraction analysis and computational studies indicate

30 ven of them have been characterized by X-ray diffraction analysis and the C18 columnar packing compar

31 Detailed electron diffraction analysis combined with first-principles calc

32 ing curve in molybdenum by synchrotron X-ray diffraction analysis of crystalline microstructures, gen

33 Single-crystal X-ray diffraction analysis of the monomers confirmed that they

34 In situ X-ray diffraction analysis reveals that the material undergoes

35 X-ray diffraction analysis showed that calcium carbonate is fo

36 Single crystal X-ray diffraction analysis shows that host-guest interactions

37 In situ single-crystal X-ray diffraction analysis was carried out at 298 K using an e

38 by multinuclear NMR and single-crystal X-ray diffraction analysis.

39 in ternary adduct was characterized by X-ray diffraction analysis.

40 plex was prepared and characterized by X-ray diffraction analysis.

41 r scale, confirmed through synchrotron-based diffraction and aberration corrected electron microscopy

42 uded transmission electron microscopy, X-ray diffraction and asymmetrical flow field-flow fractionati

43 Through high-energy x-ray diffraction and atomic pair density function analysis we

44 and confirmed in our experiments using X-ray diffraction and atomic resolution STEM-HAADF electron mi

45 Here, we integrate high pressure X-ray diffraction and atomistic simulations to correlate the a

46 er X-ray diffraction, selected area electron diffraction and electron microscopy imaging.

47 Surface plasmon resonance diffraction and electrophoretic mobility shift assays we

48 lution of the metal sulfide-utilizing powder diffraction and fluorescence imaging to resolve the form

49 The X-ray powder diffraction and FTIR analyses showed a significant reduc

50 We present combined in situ X-ray diffraction and high-speed imaging to monitor the phase

51 By means of single crystal neutron diffraction and inelastic neutron scattering experiments

52 Neutron diffraction and inelastic neutron scattering studies ena

53 ntial scanning calorimetry, wide angle X-ray diffraction and infrared spectroscopy.

54 g the release step, as demonstrated by X-ray diffraction and mechanical modeling.

55 Using in situ neutron diffraction and meta-dynamic simulation, we discovered t

56 he temporal resolution of ultrafast electron diffraction and microscopy experiments is currently limi

57 ures over 2,500 K using single-crystal X-ray diffraction and Mossbauer spectroscopy in laser-heated d

58 By combining neutron diffraction and muon spin relaxation on a stoichiometric

59 e and solutions were established using X-ray diffraction and NMR spectroscopy.

60 X-ray diffraction and optical studies demonstrate that superhy

61 teractions were studied by High-Energy X-ray Diffraction and Pair Distribution Function (PDF) analysi

62 telluride as a test case, we performed X-ray diffraction and Raman scattering experiments to benchmar

63 X-ray diffraction and reciprocal space maps identify the in-pl

64 Synchrotron X-ray powder diffraction and Rietveld refinement were then used to el

65 onfirm its structure by single-crystal X-ray diffraction and show by (27) Al NMR spectroscopy, electr

66 A historical challenge: Gas-phase electron diffraction and single-crystal X-ray diffraction are bot

67 In the present study neutron diffraction and small-angle neutron scattering measureme

68 materials quality, as characterized by X-ray diffraction and surface area analysis.

69 indicate the detection limit of synchrotron diffraction and TEM.

70 The combination of Bragg diffraction and tfPDF provides a much more complete desc

71 rokaryotic membranes using synchrotron x-ray diffraction and that it is sufficient to kill S. aureus

72 Through synchrotron x-ray powder diffraction and tomography measurements, uranium dioxide

73 X-ray diffraction and transmission electron microscopy charact

74 oprobe) and structural (electron backscatter diffraction and transmission electron microscopy) charac

75 rmined by a combination of X-ray and neutron diffraction and was confirmed with solid-state (31) P NM

76 aracterization using synchrotron-based X-ray diffraction and X-ray absorption spectroscopy.

77 Through X-ray diffraction and X-ray photoelectron spectroscopy, the as

78 e spectrum elemental line scan, X-ray powder diffractions and Raman spectroscopy.

79 orescence spectroscopy, single-crystal X-ray diffraction, and cyclic voltammetry.

80 ay absorption fine structure, neutron powder diffraction, and density functional theory calculations.

81 n electron microscopy, high resolution X-ray diffraction, and electron channeling contrast imaging.

82 ling microscopy, high-pressure surface X-ray diffraction, and high-pressure vibrational spectroscopy.

83 opy and low-temperature single-crystal X-ray diffraction, and in the gas phase by quantum-chemical ca

84 magnetic ferroelectric Mn2GeO4 using neutron diffraction, and show that it features a double-Q conica

85 n law derivations, these derivations include diffraction, and so are valid also for small objects, an

86 the applied voltage, resulting in switchable diffraction angles.

87 brane proteins display systematically higher diffraction anisotropy than those of soluble proteins.

88 lectron diffraction and single-crystal X-ray diffraction are both established techniques, but they we

89 ine ligands and single crystal X-ray/neutron diffraction are exploited in tandem to allow structural

90 We used low-angle x-ray diffraction at the European Synchrotron Radiation Facili

91 that generate coherent light well below the diffraction barrier bringing fundamentally new capabilit

92 or of 2.5 less than for single-crystal X-ray-diffraction-based structure determination.

93 ed to exactly balance both the repulsion and diffraction-broadening.

94 onally difficult to characterize by standard diffraction, can be elucidated using tfPDF.

95 Optical, electrochemical, and X-ray diffraction characterization of 3,7- and 2,6-dithienyl-s

96 From X-ray diffraction, charge transport (electrical resistivity, H

97 We have used operando X-ray diffraction computed tomography (XRD-CT) to study specif

98 Single-crystal X-ray diffraction confirmed structures that resemble a spinnin

99 ectron microscopy and selected-area electron diffraction confirmed that all solids precipitated withi

100 scillations at medium- and substrate-related diffraction cut-off edges.

101 erver takes primary sequence and raw crystal diffraction data as input, with output containing annota

102 temperature and Rietveld analyses of neutron diffraction data at low temperature indicate that exposu

103 ith the presence of defined multimers, X-ray diffraction data in solution and negative-stain electron

104 Rietveld refinements of the in situ neutron diffraction data indicate that the actual transformation

105 We show from high-resolution powder neutron diffraction data that the high-temperature phase has zer

106 uctural analysis with X-ray crystallographic diffraction data to 2.0-A revealed that each protein sub

107 situ synchrotron and time-of-flight neutron diffraction data to retain the P213 space group, though

108 TTPA was crystallized and X-ray diffraction data were collected to a resolution of 1.9 A

109 esolution structures, required deposition of diffraction data, and improved methods for discriminatin

110 ed by Landau theory and single-crystal X-ray diffraction data, we re-evaluate the space group symmetr

111 fs and call for a specific handling of their diffraction data.

112 mpleteness, as well as the resolution of the diffraction data.

113 d has been suggested as a way of phasing the diffraction data.

114 acterization by high-resolution powder X-ray diffraction, density functional theory calculation and a

115 microanalysis (EPMA), electron backscattered diffraction (EBSD) combined with energy-dispersive elect

116 We have applied the electron backscatter diffraction (EBSD) technique in a scanning electron micr

117 obtained by post-mortem electron backscatter diffraction (EBSD).

118 ave optics model to account for the dominant diffraction effect at this new scale, and the system poi

119 These structures exhibit high diffraction efficiencies over a broad range of angles of

120 2) The required voltage to achieve peak diffraction efficiency (eta 32%) for the 1(st) order is

121 multiplex and label-free fashion by means of diffraction efficiency changes.

122 e control of macroscopic optical density and diffraction efficiency of the BD texture is demonstrated

123 ption and are phase-only holograms with high diffraction efficiency.

124 ehensive structural characterizations (X-ray diffraction, electron microscopy, Raman, and UV-visible

125 Methods such as diffraction, endoscopy, and optical coherence tomography

126 allows accessing much shorter timescales in diffraction experiments at synchrotron sources.

127 In situ X-ray diffraction experiments can provide insights into the dy

128 Here we present X-ray diffraction experiments with femtosecond resolution that

129 ied through spectral measurements, far-field diffraction experiments, and thermal imaging.

130 3O9N produces a minimal background in powder diffraction experiments, and was therefore exploited for

131 R, molecular dynamics calculations and X-ray diffraction experiments, we demonstrated that these thre

132 logy, as accessed by grazing incidence X-ray diffraction experiments.

133 olid-state NMR spectroscopy and powder X-ray diffraction experiments.

134 yo-electron microscopy method micro-electron diffraction explain its dominant influence on tau aggreg

135 The characteristics of the generated diffraction-free array including its period, propagation

136 chanics and micrometer-nanometer-scale X-ray diffraction from synchrotron light in intact ventricular

137 ak sidelobes approaches the limit imposed by diffraction from the finite field extent in the grating

138 processes, as demonstrated by in situ X-ray diffraction, galvanostatic intermittent titration techni

139 As a result, a two-dimensional polarization diffraction grating is formed that generates six differe

140 n on the intensity of the central light-wave diffraction grating was used to determine the molecular

141 Polarized and unpolarized neutron diffractions have been carried out to investigate the na

142 Our X-ray diffraction, high-resolution transmission electron micro

143 structure has been confirmed by powder X-ray diffraction, high-resolution transmission electron micro

144 Via 2D X-ray diffraction, highly ordered and textured crystals for fi

145 X-ray fibre diffraction, hydrogen-deuterium exchange and solid-state

146 Electron diffraction identified the original cerium oxide particl

147 ndly software to process the collected X-ray diffraction images makes the technique accessible to a w

148 Coherent diffraction imaging (CDI) in the extreme ultraviolet has

149 5,Fe0.25)SiO3 using synchrotron radial X-ray diffraction in a membrane-driven laser-heated diamond an

150 Using synchrotron x-ray diffraction in diamond anvil cells and multiscale simula

151 ntly reports antibiotic binding and provides diffraction information in determining the structure wit

152 image, accurately assembling them into a 3D diffraction intensity function, and determining missing

153 ers of magnitude of sharp increases in X-ray diffraction intensity.

154 Coherent x-ray diffraction investigations on Ag five-fold twinned nanow

155 The achievable resolution for Larmor diffraction is comparable to that using Neutron Resonanc

156 this concentration-dependent coherent light diffraction is due to the ultrafast and large third-orde

157 chrotron radiation-based high-pressure X-ray diffraction is used to quantify the influence of dreierk

158 construction is ultimately determined by the diffraction limit for the wavelength of the radiation us

159 ing either model has been constrained by the diffraction limit of light microscopy, as the cisternae

160 these structures lie at or below the 250 nm diffraction limit of light microscopy.

161 ion microscopy (SMLM) optically overcame the diffraction limit of light to resolve fluorescently labe

162 y allows optical imaging below the classical diffraction limit of light with currently up to 20x high

163 the samples are often below or close to the diffraction limit of the probe light.

164 urring at length scales smaller than light's diffraction limit.

165 can study particles smaller than the optical diffraction limit.

166 rganization and dynamics in cells beyond the diffraction limit.

167 tosis, but the size of vesicles is below the diffraction limit.

168 ate electromagnetic wave distribution in the diffraction limit.

169 in nanoscale structures operating below the diffraction limit.

170 hip integrated logic circuits overcoming the diffraction limitation of photonics.

171 ed and live cells (human MRC5 lung cells) in diffraction limited and super-resolved fluorescence micr

172 s confirmed that imprinted probes enable sub-diffraction limited imaging with a spatial resolution co

173 assembled into meta-surfaces to generate any diffraction-limited acoustic field.

174 longitudinal modes with a single lobe, near-diffraction-limited far field.

175 rum, and summarize their important features: diffraction-limited focusing, high-quality imaging, and

176 rements of spatially-diverse field patterns, diffraction-limited images of human-sized subjects are r

177 with the fitted phase plate the optics shows diffraction-limited performance, generating a nearly Gau

178 nt of cargo vesicles whose size is below the diffraction-limited resolution of the optical microscope

179 localizing individual nanoparticles within a diffraction-limited spot.

180 des to free-space beams forming micron-scale diffraction-limited spots a designed distance and angle

181 and imaging are demonstrated, revealing sub-diffraction-limited topographic features.

182 al resolution far below conventional optical diffraction limits.

183 , Cl (4)) were studied by gas-phase electron diffraction, low-temperature NMR spectroscopy, and high-

184 Here, using three-dimensional (3D) electron diffraction mapping approach, we non-destructively explo

185 Our study demonstrates that 3D electron diffraction mapping is a powerful tool for the cross-sec

186 Coupled with X-ray diffraction mapping, GFA is determined from direct R C m

187 Electron diffraction measured tendril growth axes and grain bound

188 the first principle calculation and neutron diffraction measurement.

189 4(+*)) were examined by single-crystal X-ray diffraction measurements and density functional theory c

190 Synchrotron x-ray diffraction measurements demonstrate that there is a sig

191 The diffraction measurements indicate that all four MOFs ads

192 Here we show in situ pump-probe X-ray diffraction measurements on fused silica crystallizing t

193 provide insight into dynamic processes where diffraction methods fail.

194 The combination of spectroscopic and diffraction methods to study chemical transformations is

195 rystal-structure prediction and powder X-ray diffraction methods, we identified this elusive phase as

196 ementary use of neutron, X-ray, and electron diffraction methods.

197 By combining x-ray diffraction, molecular dynamics simulations, and electro

198 sed micro X-ray fluorescence (mu-XRF), X-ray diffraction (mu-XRD), and scanning transmission X-ray mi

199 urier transform infrared spectroscopy, x-ray diffraction, native electrophoresis, and electron micros

200 e, requiring tracking of rapidly moving, sub-diffraction objects in a crowded, noisy environment.

201 Single-crystal X-ray diffraction of its tris(cobaltocenium) salt ([(+)-NDI-De

202 ated beam quality due to multimode behavior, diffraction of light and self-focusing.

203 X-ray diffraction of precipitates showed that Mnt interlayer s

204 The low diffraction of the Bessel beam coupled with the ability

205 Neutron diffraction of tri(3,5-tert-butylphenyl)methane at 20 K

206 tion-selective flat waveplates, and adaptive diffraction optics.

207 In our design, the 1(st) diffraction order occurs at 4.3 degrees , while the 2(nd

208 sample was characterized using powder X-ray diffraction (p-XRD) and scanning electron microscopy (SE

209 S, TGA-MS, high resolution synchrotron X-ray diffraction, pair distribution function analysis, Raman,

210 The diffraction pattern of a DOE is highly sensitive to the

211 comparing and fitting the experimental X-ray diffraction pattern with Debye formula simulated pattern

212 ron microscopy, UV-Visible spectra and X-ray diffraction pattern.

213 zigzag-shaped pattern yields crescent-shaped diffraction pattern.

214 The diffraction patterns by Abeta1-28WT and Abeta1-28A2V ass

215 lasers now have the ability to collect X-ray diffraction patterns from individual molecules; however,

216 fferent protein samples by merging pink-beam diffraction patterns from many crystals, each collected

217 le acquiring consecutive in situ synchrotron diffraction patterns from the beginning to the end of th

218 o-dimensional X-ray Bragg coherent intensity diffraction patterns measured at a single incident beam

219 act disk drive, was developed to measure the diffraction patterns of these biogratings, thus allowing

220 e local radiation damage that is seen in the diffraction patterns of these objects and has been sugge

221 The analysis of the diffraction patterns shows that the structural order of

222 systematic change in shape and intensity of diffraction patterns with increasing addition of salt co

223 eplacement already converges in 1,000-10,000 diffraction patterns, which we collected in 3 to maximal

224 um long crack has been analyzed through Laue diffraction peak shapes.

225 by analyzing the intensity ratio between two diffraction peaks from two-dimensional slabs of the vari

226 Fabrics displaying higher-order diffraction peaks in the visible regime were produced fr

227 te of 1.8 frames/s by using epi-illumination diffraction phase microscopy (epi-DPM).

228 The phase conjugated diffraction property from the recorded nanostructures wa

229 from N2 -physisorption and rotation electron diffraction provide evidence for the openness of the 12

230 rization of the samples include powder X-ray diffraction (pXRD), scanning electron microscopy (SEM) a

231 d by transmission electron microscopy, X-ray diffraction, Raman spectroscopy, X-ray photoelectron spe

232 the ceria particles had additional electron diffraction reflections indicative of a CeO2 superstruct

233 n situ time-resolved synchrotron-based X-ray diffraction, remarkably agreeing with the sorption isoth

234 quenching boundaries all-optically with sub-diffraction resolution, thus characterizing spatiotempor

235 o2(p-dobdc) via in situ single-crystal X-ray diffraction reveal that the vast improvement in selectiv

236 Single-crystal X-ray diffraction revealed a triclinic crystal with unit cell

237 xTex superconductors, bulk-sensitive neutron diffraction revealed an in-plane oriented diagonal doubl

238 ral characterization by single-crystal X-ray diffraction reveals that these compounds adopt an unprec

239 ucture, investigated by single-crystal X-ray diffraction, reveals the formation of a three-dimensiona

240 out by different techniques including X-ray diffraction, scanning electron microscopy, transmission

241 films were analyzed by electron backscatter diffraction, scanning transmission electron microscopy,

242 of a new spatial periodicity below TDW from diffraction, scanning tunnelling and photoemission based

243 eptionally narrow rocking curve in the X-ray diffraction scans as well as from scanning transmission

244 roborated using in situ single-crystal X-ray diffraction (SCXRD) studies.

245 l prisms was concluded based on powder X-ray diffraction, selected area electron diffraction and elec

246 X-ray diffraction showed the presence of apatite in both donor

247 to (Ph3P)6Cu6H6 and by microanalysis; X-ray diffraction shows that the complex is a bitetrahedron in

248 stribution combining with kinematic electron diffraction simulation confirms that for such a Ag FTNW,

249 mparing the same with the dynamical electron diffraction simulations.

250 l slabs of the various phases, determined by diffraction simulations.

251 analyzed for polymorphism using powder X-ray diffraction, solid fat content by pulsed nuclear magneti

252 X-ray diffraction structures of oxidoreductase flavoenzymes ha

253 In situ synchrotron X-ray diffraction studies were conducted in the Cs/Sn/P/Se sys

254 may offer in these and similar time-resolved diffraction studies.

255 pectrometry independently verifies the X-ray diffraction study based heavy atoms formula, Au279S84, a

256 A neutron diffraction study of cholesterol oxidase has revealed an

257 Here, utilizing the synchrotron X-ray diffraction technique, we for the first time, experiment

258 vercome the limitations of X-ray and neutron diffraction techniques and makes possible, in principle,

259 t be identified using the conventional Bragg diffraction techniques traditionally used to study cryst

260 Compared to existing analogous X-ray diffraction techniques, ToF 3DND enables studies of samp

261 ochemical impedance spectroscopy and neutron diffraction, these results show that the lattice softnes

262 s been characterized by single-crystal X-ray diffraction, thus demonstrating the capability of the gi

263 by the method of single-wavelength anomalous diffraction to 2.31 A resolution.

264 ing synchrotron-based grazing incident X-ray diffraction to observe crystal structure and chemical tr

265 John was first to use X-ray diffraction to solve the 3-dimensional structure of a pr

266 sis (fwhm) was performed on the powder X-ray diffraction traces and showed that the higher concentrat

267 X-ray diffraction tracks the light-induced femtosecond coheren

268 l scanning calorimetry, single-crystal X-ray diffraction, transient absorption spectroscopy, theoreti

269 udied using a combination of in-situ neutron diffraction, transmission electron microscopy and modell

270 and purity were verified using powder X-ray diffraction, transmission electron microscopy, Raman and

271 Dynamically, ultrafast electron diffraction (UED) with atomic-scale spatiotemporal resol

272 Despite its short history, diffraction-unlimited fluorescence microscopy techniques

273 ution scanning TEM (STEM) and single-crystal diffraction using synchrotron radiation.

274 ectron microscopy, elemental analysis, X-ray diffraction, UV-visible (UV-vis) and Fourier transform i

275 l phase modulation and the non-local lattice diffraction via inverse scattered field and geometry opt

276 High temperature X-ray diffraction was used to detail the kinetics of perovskit

277 Selected area diffraction was used to elucidate the hexagonal crystal

278 Using the cryoEM method microelectron diffraction, we determined the atomic structures of 11-r

279 Using wide Q-range liquid-phase neutron diffraction, we elucidate the mechanism of reaction at a

280 he weaving process with single crystal X-ray diffraction, we find that the degree of polymerization a

281 led with fluorescence spectroscopy and X-Ray diffraction, we report here that this disparity is inste

282 tu high-pressure synchrotron radiation X-ray diffraction, we reveal a polymorphic transition from fac

283 Raman spectroscopy and X-ray diffraction were further employed to interrogate the mat

284 zed Light Thermomicroscopy, and Powder X-ray Diffraction were used in investigation.

285 olymer single crystals are analyzed by X-ray diffraction, which is the first case of a scsc two-dimen

286 nning calorimetry, and high resolution X-ray diffraction with refinement fitting.

287 aled by joint studies with synchrotron X-ray diffraction, X-ray absorption fine structure, neutron po

288 NU-1000 using synchrotron-based X-ray powder diffraction, X-ray absorption, and infrared spectroscopy

289 mic force microscopy, grazing incident X-ray diffraction, X-ray photoelectron spectroscopy, and Fouri

290 energy-dispersive X-ray spectroscopy, X-ray diffraction, X-ray photoelectron spectroscopy, and nitro

291 ossbauer, magnetometry, single crystal X-ray diffraction, XAS, and EXAFS for 6.

292 microscopy (SEM), UV-Vis spectroscopy, X-ray diffraction (XRD) analysis and Fourier transform infra-r

293 d in the solid state by single-crystal X-ray diffraction (XRD) and in solution using multinuclear NMR

294 ilot study examines the correlation of X-ray diffraction (XRD) measurements with the histopathologica

295 The X-ray diffraction (XRD) pattern at 0.84 GPa suggests that the

296 RS determination and X-ray diffraction (XRD) were used to evaluate the influence of

297 , vibrating sample magnetometer (VSM), X-ray diffraction (XRD), and X-ray photoelectron spectroscopy

298 1 and 2:1) was proved by experimental (X-ray diffraction (XRD), thermal gravimetric analysis (TGA), (

299 electron microscopy (SEM), and in situ X-ray diffraction (XRD).

300 x-ray diffraction(XRD) tests demonstrated the intermetallics w